中国化学会第十二届全国分析化学年会(第一轮通知)

中国化学会和国家自然科学基金委主办、华中师范大学承办的"第十二届全国分析化学年会"定于2015年5月8日至11日在武汉洪山大礼堂召开。这是我国分析化学领域三年一届的盛会,会议将就我国自上届学术会议以来分析化学     

基于纳米Zr3Y2O9交叉敏感的苯和三甲胺传感器

基于纳米Zr3Y2O9对苯和三甲胺的催化发光有交叉敏感现象,建立了同时测定空气中苯和三甲胺的新方法。在两个波长处分别确定苯和三甲胺的响应关系,再通过两个波长处的叠加发光信号准确获取苯和三甲胺的浓度。最佳实验条件为:两个分析波长分别为440和540 nm,敏感材料表面温度313℃,载气流速140 mL/min。方法的检出限(3σ)分别为苯(440 nm)0.30 mg/m3和三甲胺(540 nm)0.70 mg/m3,线性范围分别为苯(440 nm)0.8~105.0 mg/m3、苯(540 nm)3.0~130.0 mg/m3、三甲胺(440 nm)2.5~232.0 mg/m3和三甲胺(540 nm)1.2~156.0 mg/m3,回收率为苯96.8%~102.3%和三甲胺97.6%~103.4%。常见共存物(甲醛、乙醇、丙酮、氨、二氧化硫和二氧化碳等)不干扰测定。连续200 h通浓度均为50 mg/m3的苯和三甲胺混合气体,发光强度的相对标准偏差低于2.0%,表明此纳米级钇锆复合氧化物对苯和三甲胺的敏感性是长寿命的。本方法充分利用了交叉敏感现象,可以实现空气中苯和三甲胺的在线分析。     

金纳米粒子表面能量转移法测定水中的铅离子

荧光素修饰的凝血酶适配体(5’-FAM-GGT TGG TGT GGT TGG-3’)可与Pb2+选择性地形成G-四链体,这一构象变化能改变作为能量供体的荧光染料和作为能量受体的金纳米粒子之间的距离,使体系的荧光强度与Pb2+浓度具有一定的相关性,从而建立了一种基于纳米材料表面能量转移灵敏检测水溶液中Pb2+的分析方法。研究表明,在Pb2+浓度为12.5~100 nmol/L范围内,荧光恢复效率(F/F0)与Pb2+浓度间呈良好的线性关系,线性回归方程为y=0.910+0.007c(R2=0.997),检出限为10 nmol/L。用本方法检测自来水中Pb2+,结果令人满意。     

基于石墨烯和金纳米笼修饰的无标记型微囊藻毒素免疫传感器的研制

利用石墨烯及中空结构的金纳米笼构建了无标记型电化学免疫传感器,并用于微囊藻毒素的检测。利用多元醇还原法合成制备了导电性好、催化性强、生物相容性好的金纳米笼;再利用高分散的石墨烯将其固定于玻碳电极表面,进一步吸附固定微囊藻毒素抗体。在无微囊藻毒素存在时,电化学探针[Fe(CN)6]3!/4!在传感器界面上能获得较高的电流响应信号。当培育了微囊藻毒素后,抗体与微囊藻毒素形成免疫结合物,增加了电极表面的电荷密度和传质阻力,阻碍[Fe(CN)6]3!/4!扩散到电极表面,导致[Fe(CN)6]3!/4!的电流响应信号明显降低,电流减小的程度间接地与微囊藻毒素的浓度成比例,可实现对微囊藻毒素的检测。实验考察了抗原培育时间,抗体浓度等条件对该传感器响应性能的影响。结果表明,此传感器对微囊藻毒素的线性响应范围为0.05~1000μg/L,检出限为0.017μg/L,优于文献报道。此传感器操作简单,并且具有良好的稳定性,将其用于实际水样中微囊藻毒素的检测,平均加标回收率为94.1%。     

以一种新型Gemini表面活性剂作为介孔模板剂通过转晶过程合成介孔ZSM-5分子筛

将一种新型Gemini表面活性剂,丙撑基双(十八烷基二甲基氯化铵)[C18H37(CH3)2–N+–(CH2)3–N+–(CH3)2C18H37]Cl2(C18-3-18),作为介孔模板剂用于水热法合成介孔ZSM-5分子筛.结果表明,在130 oC低温晶化即可高效合成介孔ZSM-5分子刷.C18-3-18的加入量可影响到所合成介孔ZSM-5分子筛的相对结晶度和织构性质,它的形成遵从一个转晶过程.在合成初期,凝胶中介孔模板剂C18-3-18的使用导向了介孔材料的生成;随后在TPABr的模板作用下,介孔材料慢慢转晶生成具有MFI结构的介孔ZSM-5;然后所合成的介孔ZSM-5晶粒进一步长大并聚集形成块状颗粒,同时产生晶间介孔.C18-3-18作为介孔导向剂不仅可用于合成介孔ZSM-5分子筛,也可用于其它介孔分子筛的合成中.     

CeO2(110)负载Au纳米颗粒催化CO+NOx反应的DFT+U研究

通过在位库伦校正的密度泛函理论（DFT+U）方法计算,我们研究了CO和NO_x分子在Au负载CeO₂（110）表面的吸附. 结果表明,CO在Au纳米颗粒的顶位有很强的吸附能,大约为1.2 eV,而NO在Au纳米颗粒上或者Au与CeO₂载体界面处都是弱吸附. 然而,当NO_x在界面处形成N₂O₂二聚体之后,通过断裂末端的N-O键能够有效地被降解. 纵观整个反应过程,第一步CO+N₂O₂的反应遵循了Langmuir-Hinshelwood机理,活化能只有0.4 eV,通过形成ONNOCO的中间物种最终产生N₂O和CO₂. 不同的是,第二步消除N₂O反应遵循了Eley-Rideal碰撞机理,需要相当高的能垒,约为1.8 eV. 通过进一步分析表明,稀土Ce元素独特的电子特性能够使电子从Au上转移并且局域到载体表面的Ce阳离子上,并且有助于形成带负电的N₂O₂分子. 而且Au纳米颗粒有很强的结构流动性,能够促进吸附的CO分子靠近界面处的N₂O₂并与之反应.     

Effect of Nanoclay on the Phase Separation Behavior of Poly（methyl methacrylate）/Poly（vinyl acetate） Binary Polymer Blends

The effect of nanoclay on the phase-separation behavior of poly（methyl methacrylate）/poly（vinyl acetate）（PMMA/PVAc） blends has been mainly investigated by small-angle laser light scattering. It is found that the effect of clay on the thermodynamics and kinetics of phase-separation for PMMA/PVAc blends seems inconsistent. The kinetics phaseseparation rate decreases, while the thermodynamics parameters, cloud points Tc and delay time tD of isothermal phaseseparation also decrease, and the variation amplitude depends on the matrix composition. The affinity of clay to PMMA results in the composition difference between the border layer and the polymer matrix and further causes the concentration fluctuation at the early stage of phase separation to reduce Tc and tD. On the other hand, the decrease of phase-separation rate is caused by the mechanical barrier effect of clay on the macromolecular diffusion of blend matrix. Hence, such seemingly counterintuitive results on the thermodynamics and kinetics of phase-separation are attributed to different dominant factors.     

Vulcanization kinetics of graphene/styrene butadiene rubber nanocomposites

This paper presents the influence of graphene on the vulcanization kinetics of styrene butadiene rubber （SBR） with dicumyl peroxide. A curemeter and a differential scanning calorimeter were used to investigate the cure kinetics, from which the kinetic parameters and apparent activation energy were obtained. It turns out that with increasing graphene loading, the induction period of the vulcanization process of SBR is remarkably reduced at low graphene loading and then levels off; on the other hand, the optimum cure time shows a monotonous decrease. As a result, the vulcanization rate is suppressed at first and then accelerated, and the corresponding activation energy increases slightly at first and then decreases. Upon adding graphene, the crosslinking density of the nanocomposites increases, because graphene takes part in the vulcanization process.     

Studies on crystal transition of polyamide 11 nanocomposites by variable-temperature X-ray diffraction

Polyamide I1 （PAll） and its nanocomposites with different organoclay loadings were prepared by melt-compounding and subsequent pelletizing. The crystal phase transitions of PAl 1 and its clay nanocomposites were investigated by variable-temperature X-ray diffraction. It was found that the Brill transition of the nanocomposite was 20 K higher than that of the neat PAl 1 for both heating and cooling processes. The PAl 1 d-spacings of the nanocomposites were observed to be smaller than those of the neat PAl 1 for melt crystallization. The constraints imposed by the addition of layered clay, restricting the thermal expansion of the polymer chains, are probably responsible for such a reduction of the d-spacing.     

Electrospinning of nylon-6,6 solutions into nanofibers: Rheology and morphology relationships

The relationship between the rheological properties of nylon-6,6 solutions and the morphology of their electrospun nanofibers was established. The viscosity of nylon-6,6 in formic acid(90%) was measured in the concentration range of 5 wt%-25 wt% using a programmable viscometer. Electrospinning of nylon-6,6 solutions was carried out under controlled parameters. The chemical structure, morphology and thermal properties of the obtained nanofibers were investigated using Fourier transform infrared spectroscopy(FTIR), scanning electron microscopy(SEM) and differential scanning calorimetry(DSC), respectively. Entanglement concentration(ce) was found to be 15 wt% and a power law relationship between specific viscosity and solution concentration was observed with exponents of 2.0 and 3.3 for semi-dilute unentangled(c ce) and semi-dilute entangled(c ce) regimes, respectively. The diameter and uniformity of the nanofibers were found to be dependent on the viscosity. Moreover, the average diameter of electrospun nanofibers was found to be dependent on zero shear rate viscosity and normalized concentration(c/ce) in a power law relationship with exponents of 0.298 and 0.816, respectively. For nylon-6,6 solutions, the entanglement concentration(ce = 15 wt%) provides the threshold viscosity required for the formation of a stable polymeric jet during electrospinning and producing uniform beadless fibers. For concentrations less than ce, beaded fibers with some irregularities are formed. DSC analysis showed an increase in crystallinity of all electrospun samples compared to original polymer. Furthermore, Based on FTIR spectroscopy, α phase is dominant in electrospun nanofibers and minor amount of β and γ phases is also available.